Zoom lens

ABSTRACT

Disclosed is a zoom lens comprising at least three movable lens units. The zoom lens comprises a first lens unit disposed closest to an object side and having positive refractive force. The first lens unit includes a positive cemented lens constituted by a positive lens element and a negative lens element, with a concave side of the cemented surface facing the object side. The zoom lens also comprises a last lens unit disposed closest to an image side. Upon zooming from a wide angle end to a telephoto end, at least the first lens unit and the last lens unit move toward the object side so as to increase an air gap between the first lens unit and a lens unit adjacent to the first lens unit on the image side but to decrease an air gap between the last lens unit and a lens unit adjacent to the last lens unit on the object side. The zoom lens satisfies the following condition: 0.7&lt;f1/(fwxft)+E,fra 1/2+EE &lt;1.4 where f1 is the focal length of the first lens unit, fw is the focal length of the entire lens system at the wide angle end, and ft is the focal length of the entire lens system at the telephoto end.

This is a division of application Ser. No. 08/363,339 filed Dec. 23,1994 now U.S. Pat. NO. 5,606,460.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates generally to a zoom lens and, moreparticularly, to a zoom lens suitable for use with a lens shutter typecamera or the like.

2. Related Background Art

In recent years, a zoom lens has been dominated in the sector ofphotographing lenses of a lens shutter type camera.

Also, with a higher performance of the zoom lens, a variety of zoomtypes have been proposed. Further, because of an advancement oftechnology for a lens barrel in recent years, there have been proposed avariety of zoom types in which high zoom ratio is attained by use of azoom lens constructed of three or more movable lens units, a so-calledmulti-unit zoom lens.

Given first is a generality about the multi-unit zoom lens including thethree or more movable lens units.

In the multi-unit zoom lens, there increases freedom for selecting azooming locus of each lens unit upon zooming from a wide angle end to atelephoto end, and, therefore, freedom in terms of correcting anaberration also increases. Further, because lens units changingmagnification for zooming are increased, it is possible to attain ahigher performance while increasing a zooming ratio. There has hithertoexisted a problem in which a structure of a lens barrel becomesintricate with an increment in the number of movable elements. Thisproblem is, however, overcome to some extent owing to the advancement ofthe technology for the lens barrel in recent years.

Hitherto, in the zoom lens with no restriction of a back focus, anegative lens unit has been disposed closest to an image side in orderto reduce the total length of the lens system and to make the lens sizesmall. The zooming is effectively performed by augmenting a variation inthe back-focal distance upon zooming from the wide angle end to thetelephoto end.

Further, a positive lens unit is disposed closest to the object side inthe lens system, thereby attaining the reduction in the total length atthe telephoto end.

From the above, a positive/positive/negative 3-unit zoom lens and apositive/negative/positive/ negative 4-unit zoom lens may bespecifically cited as a multi-unit zoom lens capable of increasing thezoom ratio and suitable for the down-sizing, and a variety of proposalspertaining thereto have been made.

The positive/positive/negative 3-unit zoom lens is constructed of,sequentially from the object side, a first lens unit having refractivepower, a second lens unit having the positive refractive power and athird lens unit having negative refractive power. This zoom lens isconstructed so as to, upon zooming from the wide angle end to thetelephoto end, increase an air gap between the first lens unit and thesecond lens unit but to decrease an air gap between the second lens unitand the third lens unit (e.g., Japanese Patent Application Laid-Open No.2-73211).

On the other hand, the positive/negative/positive/negative zoom lens isconstructed of, sequentially from the object side, a first lens unithaving the positive refractive power, a second lens unit having thenegative refractive power, a third lens unit having the positiverefractive power and a fourth lens unit having the negative refractivepower. This zoom lens is constructed so as to, upon zooming from thewide angle end to the telephoto end, increase an air gap between thefirst lens unit and the second lens unit but to decrease both an air gapbetween the second lens unit and the third lens unit and an air gapbetween the third lens unit and the fourth lens unit (e.g., JapanesePatent Application Laid-Open No. 3-39920). Also, in the zoom lens withno restriction in terms of the back-focal distance that is used for alens shutter type camera, it is required for attaining the down-sizingof the camera body to reduce both a size of each lens and a thickness ofthe lens system (collapse lens thickness) when collapsed in the camerabody. In this case, there are reduced both a length (total lensthickness) of the lens system along an optical axis extending from theclosest-to-object surface to the closest-to-image surface and athickness of each lens unit. These reductions are effective in thedecrease in the collapse lens thickness and, in turn, the down-sizing ofthe camera body.

However, in the conventional multi-unit zoom lens such as thepositive/positive/negative 3-unit zoom lens and thepositive/negative/positive/negative 4-unit zoom lens, the negative lenselement of the first lens unit is disposed closest to the object side inorder to well correct a positive distortion at the wide angle end andobtain a sufficient back-focal distance. Then, if the first lens unit isconstructed of two lens elements, a negative spherical aberration isinsufficiently corrected. A well-corrected negative spherical aberrationentails nothing but to increase the number of the constructive lenselements or to make the lens surface aspherical. As a result, therearises an inconvenience of being insufficient in terms of simplifyingthe configuration and reducing the costs.

SUMMARY OF THE INVENTION

It is a primary object of the present invention, which was devised inview of the problems given above, to provide a zoom lens exhibiting anexcellent imaging performance while simplifying a configuration,reducing costs and attaining down-sizing.

According to one aspect of the present invention, there is provided azoom lens comprising: at least three pieces of movable lens unitsincluding a first lens unit G1 disposed closest to an object side andhaving positive refractive force and a last lens unit GE disposedclosest to an image side. It would be preferable that the last lens unithave negative refractive power. Upon zooming from a wide angle end to atelephoto end, at least the first lens unit G1 and the last lens unit GEmove toward the object side so as to increase an air gap between thefirst lens unit G1 and a lens unit adjacent to the first lens unit G1 onthe image side but to decrease an air gap between the last lens unit GEand a lens unit adjacent to the last lens unit GE on the object side.The first lens unit G1 includes a positive cemented lens L1 constitutedby a positive lens element L11 and a negative lens element L12, with aconcave side of the cemented surface facing the object side. The zoomlens satisfies the following condition:

    0.7<f1/(fw·ft).sup.1/2 <1.4

where f1 is the focal length of said first lens unit, fw is the focallength of the entire lens system at the wide angle end, and ft is thefocal length of the entire lens system at the telephoto end.

According to another aspect of the present invention, there is provideda zoom lens comprising in the following order from the object side: afirst lens unit G1 having positive refractive power, a second lens unitG2 having the positive refractive power and a last lens unit GE havingnegative refractive power. Upon zooming from a wide angle end to atelephoto end, at least the first lens unit G1 and the last lens unit GEmove toward the object side so as to increase an air gap between thefirst lens unit G1 and the second lens unit G2 but to decrease an airgap between the second lens unit G2 and the last lens unit GE.

According to still another aspect of the present invention, there isprovided a zoom lens comprising in the following order from the objectside: a first lens unit G1 having positive refractive power, a secondlens unit G2 having negative refractive power; a third lens unit G3having the positive refractive power; and a last lens unit GE having thenegative refractive power. Upon zooming from a wide angle end to atelephoto end, at least the first lens unit G1 and the last lens unit GEmove toward the object side so as to increase an air gap between thefirst lens unit G1 and the second lens unit G2 but to decrease both anair gap between the second lens unit G2 and the third lens unit G3 andan air gap between the third lens unit G3 and the last lens unit GE.

According to yet another aspect of the present invention, there isprovided a zoom lens comprising in the following order from the objectside: a first lens unit G1 having positive refractive power; a secondlens unit G2 having negative refractive power; a third lens unit G3having the positive or negative refractive power; a fourth lens unit G4having the positive refractive power; and a last lens unit GE having thenegative refractive power. Upon zooming from a wide angle end to atelephoto end, at least the first lens unit G1 and the last lens unit GEmove toward the object side so as to increase an air gap between thefirst lens unit G1 and the second lens unit G2 but to decrease an airgap between the fourth lens unit G4 and the last lens unit GE.

In the zoom lens according to any aspect of the present invention, thefirst lens unit G1 includes a positive cemented lens L1 constituted by apositive lens element L11 and a negative lens element L12, with aconcave side of a cemented surface facing the object side. The zoom lenssatisfies the following condition:

    0.7<f1/(fw·ft).sup.1/2 <1.4

where f1 is the focal length of the first lens unit G1, fw is the focallength of the entire lens system at the wide angle end, and ft is thefocal length of the entire lens system at the telephoto end.

According to a preferable mode of the present invention, the zoom lenssatisfies the following conditions:

    0.08<fw·(N1n-N1p)/|r1m|<0.5

    35<(ν1p-ν1n)

where fw is the focal length of the entire lens system at the wide angleend, N1p is the refractive index of the positive lens element L11 in thefirst lens unit G1 with respect to the d-line, N1n is the refractiveindex of the negative lens element L12 in the first lens unit G1 withrespect to the d-line, ν1p is the Abbe number of the positive lenselement L11 in the first lens unit G1 with respect to the d-line, ν1n isthe Abbe number of the negative lens element L12 in the first lens unitG1 with respect to the d-line, and r1m is the radius of curvature of thecemented surface in the first lens unit G1.

The zoom lens according to the present invention is constructed of,sequentially from the object side, the first lens unit G1 having thepositive refractive power, an intermediate lens unit GA constituted byat least one lens unit and always having positive synthetic refractivepower during zooming and the last lens unit GE having the negativerefractive power.

Then, upon zooming from the wide angle end to the telephoto end, atleast the first lens unit G1 and the last lens unit GE move toward theobjects side so as to increase the air gap between the first lens unitG1 and the closest-to-object surface of the intermediate lens unit GAbut to decrease the air gap between the closest-to-image surface of theintermediate lens unit GA and the last lens unit GE.

Based on the above construction, it is possible to attain the zoom lenswhich is small both in size and in the number of its constructive lenselements but capable of increasing a zooming ratio.

Particularly, according to the present invention, the zoom ratio isincreased with a small number of lens elements. For this purpose, thefirst lens unit G1 located closest to the object side includes thecemented lens constituted by the positive lens element L11 and thenegative lens element L12, with the concave side of the cemented surfacefacing the object side, whereby a negative spherical aberration causedin the first lens unit G1 is well corrected.

As explained above, in the zoom lens with no restriction in terms of theback-focal distance, an effective layout in reducing the entire lenslength is to dispose the negative lens unit closest to the imagesurface. Hence, according to the present invention also, the last lensunit GE disposed closest to the image surface has the negativerefractive power.

Then, for attaining a much wider angle, the back-focal distance at thewide angle end is decreased to some extent, and a height of an off-axislight beam passing through the last lens unit GE is spaced away from theoptical axis. With this arrangement, an on-axis light beam and theoff-axis light beam are independently compensated.

Moreover, the reduction in the entire lens length at the wide angle endmakes it possible to decrease an effective aperture of theclosest-to-object lens surface by making the height of the off-axislight beam traveling through the first lens unit approximate to theoptical axis. Contrastingly, the back-focal distance at the telephotoend is increased, thereby making the height of the off-axis light beamspassing through the last lens unit GE more approximate to the opticalaxis than at the wide angle end. As a result, when the zooming iseffected, there increases a difference in the height of the off-axislight beam traveling through the last lens unit GE. Thus, a fluctuationin an off-axis aberration occurred in the last lens unit GE when zoomingis performed is well restrained.

The intermediate lens unit GA disposed adjacent to the first lens unitG1 on the image side includes the negative lens element L21 with itsstrong concave surface toward the object side on the closest-to-objectside. Then, at the wide angle end, the negative lens unit (syntheticlens unit of the first lens unit with the second lens unit) is disposedcloser to the object in the lens system by narrowing a spacing betweenthe first lens unit G1 and the negative lens element L21, whereby apositive distortion is well corrected. A sufficient back-focal distanceis thus obtained. Contrastingly, at the telephoto end, the divergingaction is weakened by widening the air gap between the first lens unitG1 and the negative lens element L21. This leads to the reduction in theentire lens length.

The respective conditional expressions of the present invention willhereinafter be explained.

The zoom lens according to the present invention, in addition to theabove construction, satisfies the following conditional expression (1):

    0.7<f1/(fw·ft).sup.1/2 <1.4                       (1)

where

f1: the focal length of the first lens unit G1,

fw: the focal length of the entire lens system at the wide angle end,and

ft: the focal length of the entire lens system at the telephoto end.

The conditional expression (1) prescribes a proper range of the focallength f1 of the first lens unit G1 with respect to the focal length fwat the wide angle end and the focal length ft at the telephoto end.

If above an upper limit value of the conditional expression (1), thefocal length f1 of the first lens unit G1 increases to the positive. Forthis reason, the converging action is weakened, resulting in an increasein the entire lens length at the telephoto end.

Whereas if under a lower limit value of the conditional expression (1),the focal length f1 of the first lens unit G1 decreases to the positive,and the height of the off-axis light beam passing through the first lensunit G1 is spaced away from the optical axis. Consequently, theeffective aperture of the closest-to-object lens surface increases. Itfollows that the fluctuation in the coma caused more with a larger viewangle can not be restrained.

For obtaining a much better imaging performance, it is desirable thatthe following conditional expressions (2) and (3) be satisfied:

    0.08<fw·(N1n-N1p)/|r1m|<0.5     (2)

    35<(ν1p-ν1n)                                         (3)

where

N1p: the refractive index of the positive lens element L11 in the firstlens unit G1 with respect to the d-line,

N1n: the refractive index of the negative lens element L12 in the firstlens unit G1 with respect to the d-line,

r1m: the radius of curvature of the cemented surface in the first lensunit G1,

ν1p: the Abbe number of the positive lens element L11 in the first lensunit G1 with respect to the d-line, and

ν1n: the Abbe number of the negative lens element L12 in the first lensunit G1 with respect to the d-line.

The conditional expression (2) prescribes the refractive power of thecemented surface in the first lens unit G1.

If above an upper limit value of the conditional expression (2), therefractive power of the cemented surface in the first lens unit G1becomes too large, resulting in an occurrence of a positive high-orderspherical aberration. For this reason, the first lens unit G1 can not beused bright. In the case of increasing the zoom ratio, the positivehigh-order spherical aberration increases especially at the telephotoend.

Whereas if under a lower limit value of the conditional expression (2),the refractive power of the cemented surface in the first lens unit G1becomes too small to the negative. It would be therefore difficult tocorrect the negative spherical aberration produced in the first lensunit G1.

The conditional expression (3) prescribes a difference in the Abbenumber between the positive lens element L11 and the negative lenselement L12 that constitute the positive cemented lens of the first lensunit G1.

If under a lower limit of the conditional expression (3), it is likelyto be difficult to take a balance between a correction of an on-axischromatic aberration and a correction of the negative sphericalaberration that are caused in the first lens unit G1.

For obtaining a much better imaging performance, the lens unit adjacentto the first lens unit G1 on the image side includes the negative lenselement L12 with its concave surface toward the object side on theclosest-to-object side. It is desirable that the following conditionalexpressions (4) and (5) be satisfied:

    0.7<fw·(N2n-1)/|r21|<2.0        (4)

    43<ν2n                                                  (5)

where

r21: the radius of curvature of an object-side surface of the negativelens element L21,

N2n: the refractive index of the negative lens element L21 with respectto the d-line, and

ν2n: the Abbe number of the negative lens element L21 with respect tothe d-line.

The conditional expression (4) prescribes the refractive power of theclosest-to-object surface of the lens unit adjacent to the first lensunit G1.

If above an upper limit value of the conditional expression (4), asufficient back-focal distance can be obtained at the wide angle end.There is, however, decreased a difference in the height between theon-axis light beam and the off-axis light beam that are incident on theclosest-to-object surface of the lens unit adjacent to the first lensunit G1. It would be therefore difficult to restrain the fluctuation inthe coma due to the view angle.

Whereas if under a lower limit value of the conditional expression (4),the sufficient back-focal distance can not be obtained at the wide angleend. It follows that the effective aperture of the closest-to-image lenssurface increases because of the height of the off-axis light beampassing through the last lens unit GE being spaced away from the opticalaxis.

The conditional expression (5) prescribes the Abbe number of thenegative lens element L21, disposed closest to the object side, of thelens unit adjacent to the first lens unit G1.

If under a lower limit value of the conditional expression (5), thechromatic aberration would be over-corrected off the axis than on theaxis.

Further, for attaining the down-sizing and increasing the zoom ratio,the last lens unit GE includes the positive lens element with itsconcave surface toward the object side and the negative lens elementwith its concave surface toward the object side. It is desirable thatthe following conditional expressions (6) and (7) be satisfied:

    0.35<|fe|/fw<0.85                        (6)

    0.4<ΔBf/(ft-fw)<0.85                                 (7)

where

fe: the focal length of the last lens unit GE,

and

ΔBf: the moving quantity of the last lens unit GE upon zooming from thewide angle end to the telephoto end.

The conditional expression (6) prescribes the focal length of the lastlens unit GE.

If above an upper limit of the conditional expression (6), the divergingaction of the last lens unit GE is weakened, and, hence, the height ofthe off-axis light beam passing through the last lens unit GE is toospaced away from the optical axis at the wide angle end, resulting in anaugment in the effective aperture of the closest-to-image lens surface.

Whereas if under a lower limit value of the conditional expression (6),the positive spherical aberration produced in the last lens unit GE isunder-corrected, and it follows that there increases the fluctuation inthe spherical aberration upon zooming from the wide angle end to thetelephoto end. Further, the height of the off-axis light beam travelingthrough the last lens unit GE approximates the optical axis at the wideangle end, and, therefore, it would be difficult to well restrain thefluctuation in the off-axis aberration due to the view angle.

The conditional expression (7) prescribes the moving quantity of thelast lens unit GE upon zooming from the wide angle end to the telephotoend and is associated with a rate at which the last lens unit GE takescharge of zooming when effecting the zooming.

If above an upper limit value of the conditional expression (7), thecharge-of-zooming rate of the last lens unit GE becomes too large whenperforming the zooming, it would be difficult to well correct thefluctuation in the off-axis aberration produced in the last lens unit GEwhen in the zooming.

Whereas if under a lower limit value of the conditional expression (7),the zooming burden on the last lens unit GE is relieved. Nevertheless,the charge-of-zooming rate of the lens unit adjacent to the first lensunit G1 on the image side increases. Particularly, there largely changesan angle of the off-axis light beam incident on this adjacent lens unitwhen in the zooming. For this reason, it would be difficult to wellcorrect the fluctuation in the off-axis aberration caused in theadjacent lens unit when in the zooming.

According to the present invention, upon zooming from the wide angle endto the telephoto end, the first lens unit G1 and the last lens unit GEmove together (interlocking with each other), thereby making it possibleto simplify the structure of the lens barrel.

Further, according to the present invention, it is feasible to obtainthe higher imaging performance and simplify the configuration byapplying the aspherical surface to one of the lens surfaces.

Moreover, one or a plurality of lens units are properly shifted in thedirection substantially orthogonal to the optical axis, thus correctingthe fluctuation in the image position due to a shake or the like. Aso-called vibration-reduction effect can be also acquired.

Additionally, when focusing, a preferable imaging performance can bealso obtained with respect to the objects ranging from a long range to ashort range by use of linear focus.

BRIEF DESCRIPTION OF THE DRAWINGS

Other objects and advantages of the present invention will becomeapparent during the following discussion in conjunction with theaccompanying drawings, in which:

FIG. 1 is a diagram showing a distribution of refractive power of a zoomlens and how each lens unit moves upon zooming from a wide angle end toa telephoto end in accordance with a first embodiment of the presentinvention;

FIG. 2 is a view illustrating a lens layout of the zoom lens in thefirst embodiment of this invention;

FIGS. 3A to 3D are diagrams showing various aberrations at the wideangle end in the embodiment 1;

FIGS. 4A to 4D are diagrams showing the various aberrations in anintermediate focal length state in the embodiment 1;

FIGS. 5A to 5D are diagrams showing the various aberrations at thetelephoto end in the embodiment 1;

FIG. 6 is a diagram showing a distribution of refractive power of a zoomlens and how each lens unit moves upon zooming from the wide angle endto the telephoto end in accordance with a second embodiment of thepresent invention;

FIG. 7 is a view illustrating a lens layout of the zoom lens in thesecond embodiment of this invention;

FIGS. 8A to 8D are diagrams showing various aberrations at the wideangle end in the embodiment 2;

FIGS. 9A to 9D are diagrams showing the various aberrations in anintermediate focal length state in the embodiment 2;

FIGS. 10A to 10D are diagrams showing the various aberrations at thetelephoto end in the embodiment 2;

FIG. 11 is a diagram showing a distribution of refractive power of azoom lens and how each lens unit moves upon zooming from the wide angleend to the telephoto end in accordance with a third embodiment of thepresent invention;

FIG. 12 is a view illustrating a lens layout of the zoom lens in thethird embodiment of this invention;

FIGS. 13A to 13D are diagrams showing various aberrations at the wideangle end in the embodiment 3;

FIGS. 14A to 14D are diagrams showing the various aberrations in anintermediate focal length state in the embodiment 3;

FIGS. 15A to 15D are diagrams showing the various aberrations at thetelephoto end in the embodiment 3;

FIG. 16 is a diagram showing a distribution of refractive power of azoom lens and how each lens unit moves upon zooming from the wide angleend to the telephoto end in accordance with a fourth embodiment of thepresent invention;

FIG. 17 is a view illustrating a lens layout of the zoom lens in thefourth embodiment of this invention;

FIGS. 18A to 18D are diagrams showing various aberrations at the wideangle end in the embodiment 4;

FIGS. 19A to 19D are diagrams showing the various aberrations in anintermediate focal length state in the embodiment 4; and

FIGS. 20A to 20D are diagrams showing the various aberrations at thetelephoto end in the embodiment 4.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

The present invention will hereinafter be discussed by way ofembodiments with reference to the accompanying drawings.

[Embodiment 1]

FIG. 1 is a diagram illustrating a distribution of refractive power of azoom lens and how respective lens units move upon zooming from a wideangle end to a telephoto end in a first embodiment of the presentinvention. In FIGS. 1, 6, 11 and 16, the sign represents a positive lensunit while the sign represents a negative lens unit.

As shown in FIG. 1, the zoom lens in the first embodiment is constructedof, sequentially from an object side, a first lens unit G1 havingpositive refractive power, a second lens unit G2 having the positiverefractive power and a third lens unit G3 having negative refractivepower. Then, upon zooming from the wide angle end to the telephoto end,the respective lens units move along loci indicated by arrows in theFigure so as to increase an air gap between the first lens unit. G1 andthe second lens unit G2 but to decrease an air gap between the secondlens unit G2 and the third lens unit G3.

FIG. 2 is a view illustrating a lens layout of the zoom lens inaccordance with the first embodiment of the present invention.

The zoom lens in FIG. 2 is constructed of, sequentially from the objectside, the first lens unit G1 including a positive cemented lens L1constituted by a biconvex lens and a negative meniscus lens with itsconcave surface toward the object side, the second lens unit G2including a cemented lens L21 constituted by a biconvex lens and apositive meniscus lens with its convex surface toward the object side, acemented lens L22 constituted by a biconvex lens and a negative meniscuslens with its concave surface toward the object side and a biconvex lensL23 and the third lens unit G3 including a positive meniscus lens L31with its concave surface toward the object side, a negative meniscuslens L32 with its concave surface toward the object side and a negativemeniscus lens L33 with its concave surface toward the object side.

FIG. 2 illustrates a positional relationship between the individual lensunits at the wide angle end, wherein the lens units move on an opticalaxis along the zoom loci indicated by the arrows in FIG. 1 upon zoomingto the telephoto end.

Further, a stop S is disposed in the second lens unit G2 but movestogether with the second lens unit G2 upon zooming from the wide angleend to the telephoto end.

The following Table 1 shows values of data in the embodiment 1. In Table1, f represents the focal length, FN designates the F-number, 2ω denotesthe view angle, and Bf represents the back-focal distance. Further, thesurface number indicates the order of lens surfaces from the objectside. The refractive index and the Abbe number respectively show valueswith respect to the d-line (λ=587.6 nm).

                  TABLE 1                                                         ______________________________________                                        f = 38.8-62.8-98.0                                                            FN = 4.3-5.7-7.6                                                              2ω = 58.6-36.8-24.2°                                             ______________________________________                                        Surface  Radius of                                                                              Surface    Refractive                                                                           Abbe                                      Number   Curvature                                                                              Interval   Index  Number                                    ______________________________________                                        1        39.1644  3.516      1.51860                                                                              69.98                                     2        -47.8430 1.381      1.86074                                                                              23.01                                     3        -84.1902 (d3 = variable)                                             4        -19.1336 1.256      1.74810                                                                              52.30                                     5        16.6081  3.077      1.86074                                                                              23.01                                     6        68.6075  1.884                                                       7        ∞  1.884             (stop)                                    8        213.0947 2.763      1.51680                                                                              64.10                                     9        -8.8659  1.256      1.80618                                                                              25.35                                     10       -16.2530 0.126                                                       11       100.1872 1.884      1.62041                                                                              60.14                                     12       -23.1243 (d12 = variable)                                            13       -55.4179 2.888      1.80518                                                                              25.35                                     14       -23.1413 1.381                                                       15       -33.4423 1.381      1.84042                                                                              43.35                                     16       -77.4639 3.516                                                       17       -16.8638 1.507      1.77279                                                                              49.45                                     18       -188.6525                                                                              (Bf)                                                        (Variable Interval in Zooming)                                                f       38.7909       62.7910 97.9570                                         d3      2.7697        11.4454 17.8180                                         d12     16.3041       7.6284  1.2559                                          Bf      10.5780       27.9794 51.6296                                         (Condition Corresponding Value)                                               (1) f1 / (fw · ft).sup.1/2                                                             = 1.003                                                     (2) fw · (N1n - N1p) / |r1m|                                         = 0.277                                                     (3) (ν1p - ν1n)                                                                           = 46.97                                                     (4) fw · (N2n - 1) / |r21|                                           = 1.517                                                     (5) ν2n        = 52.30                                                     (6) |fe| / fw                                                                 = 0.768                                                     (7) ΔBf / (ft - fw)                                                                       = 0.694                                                     ______________________________________                                    

FIGS. 3A to 3D, FIGS. 4A to 4D and FIGS. 5A to 5D are diagrams showingvarious aberrations respectively at the wide angle end, an intermediatefocal length state and at the telephoto end in accordance with theembodiment 1.

In each of the aberration diagrams, FN represents the F-number, Hdesignates the height of the incident light, Y denotes the image height,A designates the incident angle of the principal ray, d represents thed-line (λ=587.6 nm), and g denotes the g-line (λ=435.8 nm).

Further, in the aberration diagram showing an astigmatism, the solidline indicates the sagittal image surface S, while the broken lineindicates the meridional image surface M. More specifically, S(d) andS(g) represent the sagittal image surface with respect to the d- andg-lines, respectively. The symbols M(d) and M(g) designate themeridional image surfaces with respect to the d- and g-lines,respectively.

As obvious from the individual aberration diagrams, in this embodiment,the variety of aberrations are well corrected.

[Embodiment 2]

FIG. 6 is a diagram illustrating a distribution of refractive power of azoom lens and how respective lens units move upon zooming from a wideangle end to a telephoto end in a second embodiment of the presentinvention.

As shown in FIG. 6, the zoom lens in the second embodiment isconstructed of, sequentially from the object side, a first lens unit G1having the positive refractive power, a second lens unit G2 having thenegative refractive power, a third lens unit G3 having the negativerefractive power, a fourth lens unit G4 having the positive refractivepower and a fifth lens unit G5 having the negative refractive power.Then, upon zooming from the wide angle end to the telephoto end, therespective lens units move along loci indicated by the arrows in theFigure so as to increase both an air gap between the first lens unit G1and the second lens unit G2 and an air gap between the second lens unitG2 and the third lens unit G3 but to decrease both an air gap betweenthe third lens unit G3 and the fourth lens unit G4 and an air gapbetween the fourth lens unit G4 and the fifth lens unit G5.

FIG. 7 is a view illustrating a lens layout of the zoom lens inaccordance with the second embodiment of the present invention.

The zoom lens in FIG. 7 is constructed of, sequentially from the objectside, the first lens unit G1 including a positive cemented lens L1constituted by a biconvex lens and a negative meniscus lens with itsconcave surface toward the object side, the second lens unit G2including a biconvex lens L21 and a positive meniscus lens L22 with itsconvex surface toward the object side, a cemented lens L22 constitutedby a biconvex lens and a negative meniscus lens with its concave surfacetoward the object side and a biconvex lens L23, the third lens unit G3including a negative meniscus lens L3 with its concave surface towardthe object side, the fourth lens unit G4 including a biconvex lens L41and a cemented lens L42 constituted by a biconvex lens and a negativemeniscus lens with its concave surface toward the object side and thefifth lens unit G5 including a positive meniscus lens L51 with itsconcave surface toward the object side, a negative meniscus lens L52with its concave surface toward the object side and a negative meniscuslens L53 with its concave surface toward the object side.

FIG. 7 illustrates a positional relationship between the individual lensunits at the wide angle end, wherein the lens units move on the opticalaxis along the zoom loci indicated by the arrows in FIG. 6 upon zoomingto the telephoto end.

Further, the stop S is disposed between the third lens unit G3 and thefourth lens unit G4 but moves together with the fourth lens unit G4 uponzooming from the wide angle end to the telephoto end.

The following Table 2 shows values of data in the embodiment 2. In Table2, f represents the focal length, FN designates the F-number, 2ω denotesthe view angle, and Bf represents the back-focal distance. Further, thesurface number indicates the order of lens surfaces from the objectside. The refractive index and the Abbe number respectively show valueswith respect to the d-line (λ=587.6 nm).

                  TABLE 2                                                         ______________________________________                                        f = 39.0-83.5-112.0                                                           FN = 4.2-6.8-8.0                                                              2ω = 58.6-28.4-21.4°                                             ______________________________________                                        Surface  Radius of                                                                              Surface    Refractive                                                                           Abbe                                      Number   Curvature                                                                              Interval   Index  Number                                    ______________________________________                                        1        5.6272   4.000      1.51860                                                                              69.98                                     2        -43.3114 1.200      1.86074                                                                              23.01                                     3        -79.8455 (d3 = variable)                                             4        -33.0774 1.000      1.77279                                                                              49.45                                     5        16.5509  1.000                                                       6        16.1209  2.600      1.75520                                                                              27.61                                     7        425.6180 (d7 = variable)                                             8        -31.2898 1.000      1.77279                                                                              49.45                                     9        -94.1417 (d9 = variable)                                             10       ∞  1.500             (stop)                                    11       229.3726 1.800      1.62041                                                                              60.14                                     12       -37.7064 0.100                                                       13       29.2488  3.300      1.51860                                                                              69.98                                     14       -11.2452 1.000      1.80518                                                                              25.35                                     15       -20.9440 (d15 = variable)                                            16       -99.2788 3.000      1.80518                                                                              25.35                                     17       -21.1513 0.600                                                       18       -31.5989 1.000      1.84042                                                                              43.35                                     19       -246.0545                                                                              4.200                                                       20       -13.5005 1.500      1.77279                                                                              49.45                                     21       -95.5859 (Bf)                                                        (Variable Interval in Zooming)                                                f       39.0193       83.4643 111.9688                                        d3      2.0053        11.5430 15.3403                                         d7      3.8056        5.0756  6.3456                                          d9      3.6014        2.3314  1.0614                                          d15     15.1344       4.8474  1.7994                                          Bf      9.8804        52.5974 53.3467                                         (Condition Corresponding Value)                                               (1) f1 / (fw · ft).sup.1/2                                                             = 0.876                                                     (2) fw · (N1n - N1p) / |r1m|                                         = 0.308                                                     (3) (ν1p - ν1n)                                                                           = 46.97                                                     (4) fw · (N2n - 1) / |r21|                                           = 0.912                                                     (5) ν2n        = 49.45                                                     (6) |fe| / fw                                                                 = 0.648                                                     (7) ΔBf / (ft - fw)                                                                       = 0.559                                                     ______________________________________                                    

FIGS. 8A to 8D, FIGS. 9A to 9D and FIGS. 10A to 10D are diagrams showingvarious aberrations respectively at the wide angle end, an intermediatefocal length state and at the telephoto end in accordance with theembodiment 2.

In each of the aberration diagrams, FN represents the F-number, Hdesignates the height of the incident light, Y denotes the image height,A designates the incident angle of the principal ray, d represents thed-line (λ=587.6 nm), and g denotes the g-line (λ=435.8 nm)

Further, in the aberration diagram showing an astigmatism, the solidline indicates the sagittal image surface S, while the broken lineindicates the meridional image surface M. More specifically, S(d) andS(g) represent the sagittal image surface with respect to the d- andg-lines, respectively. The symbols M(d) and M(g) designate themeridional image surfaces with respect to the d- and g-lines,respectively.

As obvious from the individual aberration diagrams, in this embodiment,the variety of aberrations are well corrected.

[Embodiment 3]

FIG. 11 is a diagram illustrating a distribution of refractive power ofa zoom lens and how respective lens units move upon zooming from a wideangle end to a telephoto end in a third embodiment of the presentinvention.

As shown in FIG. 11, the zoom lens in the second embodiment isconstructed of, sequentially from the object side, a first lens unit G1having the positive refractive power, a second lens unit G2 having thenegative refractive power, a third lens unit G3 having the positiverefractive power and a fourth lens unit having the negative refractivepower. Then, upon zooming from the wide angle end to the telephoto end,the respective lens units move along loci indicated by the arrows in theFigure so as to increase an air gap between the first lens unit G1 andthe second lens unit G2 but to decrease both an air gap between thesecond lens unit G2 and the third lens unit G3 and an air gap betweenthe third lens unit G3 and the fourth lens unit G4.

FIG. 12 is a view illustrating a lens layout of the zoom lens inaccordance with the third embodiment of the present invention.

The zoom lens in FIG. 12 is constructed of, sequentially from the objectside, the first lens unit G1 including a positive cemented lens L1constituted by a biconvex lens and a negative meniscus lens with itsconcave surface toward the object side, the second lens unit G2including a biconvex lens L21 and a positive meniscus lens L22 with itsconvex surface toward the object side, the third lens unit G3 includinga cemented lens L32 constituted by a biconvex lens and a negativemeniscus lens with its concave surface toward the object side and thefourth lens unit G4 including a positive meniscus lens L41 with itsconcave surface toward the object side, a negative meniscus lens L42with its concave surface toward the object side and a negative meniscuslens L43 with its concave surface toward the object side.

FIG. 12 illustrates a positional relationship between the individuallens units at the wide angle end, wherein the lens units move on theoptical axis along the zoom loci indicated by the arrows in FIG. 11 uponzooming to the telephoto end.

Further, the stop S is disposed between the second lens unit G2 and thethird lens unit G3 but moves together with the third lens unit G3 uponzooming from the wide angle end to the telephoto end.

The following Table 3 shows values of data in the embodiment 3. In Table3, f represents the focal length, FN designates the F-number, 2ω denotesthe view angle, and Bf represents the back-focal distance. Further, thesurface number indicates the order of lens surfaces from the objectside. The refractive index and the Abbe number respectively show valueswith respect to the d-line (λ=587.6 nm).

                  TABLE 3                                                         ______________________________________                                        f = 38.8-62.9-110.5 mm                                                        FN = 4.0-5.5-8.0                                                              2ω = 59.0-37.6-21.8                                                     ______________________________________                                        Surface  Radius of                                                                              Surface    Refractive                                                                           Abbe                                      Number   Curvature                                                                              Interval   Index  Number                                    ______________________________________                                        1        30.1982  3.893      1.51860                                                                              69.98                                     2        -113.3634                                                                              1.381      1.86074                                                                              23.01                                     3        7,506.2080                                                                             (d3 = variable)                                             4        -23.7196 1.256      1.74810                                                                              52.30                                     5        21.8789  1.005                                                       6        22.7657  1.758      1.86074                                                                              23.01                                     7        76.8698  (d7 = variabie)                                             8        ∞  1.884      (stop)                                           9        44.3102  1.884      1.51860                                                                              69.98                                     10       -31.3119 0.126                                                       11       46.5835  3.014      1.51680                                                                              64.10                                     12       -11.7664 1.256      1.80518                                                                              25.35                                     13       -21.7079 (d13 = variable)                                            14       -48.5717 2.888      1.80518                                                                              25.35                                     15       -21.3746 0.628                                                       16       -61.7549 1.381      1.84042                                                                              43.35                                     17       -760.9659                                                                              4.395                                                       18       -13.1379 1.507      1.77279                                                                              49.45                                     19       -88.9699 (Bf)                                                        (Variable Interval in Zooming)                                                f       38.8146       62.4853 110.5160                                        d3      2.1349        9.6698  17.2047                                         d7      5.0233        3.1395  1.2558                                          d13     12.5581       6.9070  1.2558                                          Bf      11.7555       26.2929 53.6373                                         (Condition Corresponding Value)                                               (1) f1 / (fw · ft).sup.1/2                                                             = 1.077                                                     (2) fw · (N1n - N1p) / |r1m|                                         = 0.117                                                     (3) (ν1p - ν1n)                                                                           = 46.97                                                     (4) fw · (N2n - 1) / |r21|                                           = 1.224                                                     (5) ν2n        = 52.30                                                     (6) |fe| / fw                                                                 = 0.667                                                     (7) ΔBf / (ft - fw)                                                                       = 0.584                                                     ______________________________________                                    

FIGS. 13A to 13D, FIGS. 14A to 14D and FIGS. 15A to 15D are diagramsshowing various aberrations respectively at the wide angle end, anintermediate focal length state and at the telephoto end in accordancewith the embodiment 3.

In each of the aberration diagrams, FN represents the F-number, Hdesignates the height of the incident light, Y denotes the image height,A designates the incident angle of the principal ray, d represents thed-line (λ=587.6 nm), and g denotes the g-line (λ=435.8 nm).

Further, in the aberration diagram showing an astigmatism, the solidline indicates the sagittal image surface S, while the broken lineindicates the meridional image surface M. More specifically, S(d) andS(g) represent the sagittal image surface with respect to the d- andg-lines, respectively. The symbols M(d) and M(g) designate themeridional image surfaces with respect to the d- and g-lines,respectively.

As obvious from the individual aberration diagrams, in this embodiment,the variety of aberrations are well corrected.

[Embodiment 4]

FIG. 16 is a diagram illustrating a distribution of refractive power ofa zoom lens and how respective lens units move upon zooming from a wideangle end to a telephoto end in a fourth embodiment of the presentinvention.

As shown in FIG. 16, the zoom lens in the fourth embodiment isconstructed of, sequentially from the object side, a first lens unit G1having the positive refractive power, a second lens unit G2 having thenegative refractive power, a third lens unit G3 having the positiverefractive power, a fourth lens unit having the positive refractivepower and a fifth lens unit having the negative refractive power. Uponzooming from the wide angle end to the telephoto end, the respectivelens units move along loci indicated by the arrows in the Figure so asto increase an air gap between the first lens unit G1 and the secondlens unit G2, decrease an air gap between the second lens unit G2 andthe third lens unit G3, increase an air gap between the third lens unitG3 and the fourth lens unit G4 and decrease an air gap between thefourth lens unit G4 and the fifth lens unit G5.

FIG. 17 is a view illustrating a lens layout of the zoom lens inaccordance with the fourth embodiment of the present invention.

The zoom lens in FIG. 17 is constructed of, sequentially from the objectside, the first lens unit G1 including a positive cemented lens L1constituted by a biconvex lens and a negative meniscus lens with itsconcave surface toward the object side, the second lens unit G2including a biconcave lens L21 and a positive meniscus lens L22 with itsconvex surface toward the object side, the third lens unit G3 includinga biconvex lens L3, the fourth lens unit G4 including a cemented lens L4constituted by a biconvex lens and a negative meniscus lens with itsconcave surface toward the object side and the fifth lens unit G5including a positive meniscus lens L51 with its concave surface towardthe object side, a negative meniscus lens L52 with its concave surfacetoward the object side and a negative meniscus lens L53 with its concavesurface toward the object side.

FIG. 17 illustrates a positional relationship between the individuallens units at the wide angle end, wherein the lens units move on theoptical axis along the zoom loci indicated by the arrows in FIG. 16 uponzooming to the telephoto end.

Further, the stop S is disposed between the third lens unit G3 and thefourth lens unit G4 but moves together with the fourth lens unit G4 uponzooming from the wide angle end to the telephoto end.

The following Table 4 shows values of data in the embodiment 4. In Table4, f represents the focal length, FN designates the F-number, 2ω denotesthe view angle, and Bf represents the back-focal distance. Further, thesurface number indicates the order of lens surfaces from the objectside. The refractive index and the Abbe number respectively show valueswith respect to the d-line (λ=587.6 nm).

                  TABLE 4                                                         ______________________________________                                        f = 38.8-75.4-110.5 mm                                                        FN = 4.1-6.3-8.2                                                              2ω = 58.6-31.0-21.8                                                     ______________________________________                                        Surface  Radius of                                                                              Surface    Refractive                                                                           Abbe                                      Number   Curvature                                                                              Interval   Index  Number                                    ______________________________________                                        1        45.0525  3.893      1.51860                                                                              69.98                                     2        -38.2984 1.381      1.86074                                                                              23.01                                     3        -67.7399 (d3 = variable)                                             4        -21.1121 1.256      1.74810                                                                              52.30                                     5        18.7929  0.879                                                       6        18.5014  1.884      1.86074                                                                              23.01                                     7        57.8271  (d7 = variabie)                                             8        107.9504 1.758      1.51860                                                                              69.98                                     9        -25.8609 (d9 = variable)                                             10       ∞  1.884             (stop)                                    11       40.0922  3.265      1.51860                                                                              69.98                                     12       -10.7240 1.507      1.80518                                                                              25.35                                     13       -19.5245 (d13 = variable)                                            14       -149.4337                                                                              2.888      1.80518                                                                              25.35                                     15       -26.0698 1.633                                                       16       -32.9870 1.381      1.84042                                                                              43.35                                     17       -169.9714                                                                              3.767                                                       18       -16.6274 1.507      1.77279                                                                              49.45                                     19       -294.9844                                                                              (Bf)                                                        (Variable Interval in Zooming)                                                f       38.8094       75.3954 110.5159                                        d3      2.0894        11.6587 16.2726                                         d7      4.0239        2.2658  1.5123                                          d9      2.7541        4.5123  5.2657                                          d13     15.3352       5.7400  1.1521                                          Bf      9.5997        31.9941 52.0738                                         (Condition Corresponding Value)                                               (1) f1 / (fw · ft).sup.1/2                                                             = 1.008                                                     (2) fw · (N1n - N1p) / |r1m|                                         = 0.349                                                     (3) (ν1p - ν1n)                                                                           = 46.97                                                     (4) fw · (N2n - 1) / |r21|                                           = 1.375                                                     (5) ν2n        = 52.30                                                     (6) |fe| / fw                                                                 = 0.728                                                     (7) ΔBf / (ft - fw)                                                                       = 0.592                                                     ______________________________________                                    

FIGS. 18A to 18D, FIGS. 19A to 19D and FIGS. 20A to 20D are diagramsshowing various aberrations respectively at the wide angle end, anintermediate focal length state and at the telephoto end in accordancewith the embodiment 4.

In each of the aberration diagrams, FN represents the F-number, Hdesignates the height of the incident light, Y denotes the image height,A designates the incident angle of the principal ray, d represents thed-line (λ=587.6 nm), and g denotes the g-line (λ=435.8 nm).

Further, in the aberration diagram showing an astigmatism, the solidline indicates the sagittal image surface S, while the broken lineindicates the meridional image surface M. More specifically, S(d) andS(g) represent the sagittal image surface with respect to the d- andg-lines, respectively. The symbols M(d) and M(g) designate themeridional image surfaces with respect to the d- and g-lines,respectively.

As obvious from the individual aberration diagrams, in this embodiment,the variety of aberrations are well corrected.

As discussed above, according to the present invention, it is possibleto actualize the zoom lens exhibiting an excellent imaging performancewhile attaining a simplified configuration, a reduction in costs anddown-sizing as well.

It is apparent that, in this invention, a wide range of differentworking modes can be formed based on the invention without deviatingfrom the spirit and scope of the invention. This invention is notrestricted by its specific working modes except being limited by theappended claims.

What is claimed is:
 1. A zoom lens comprising in the following orderfrom the object side:a first lens unit having positive refractive powerand including a positive cemented lens having a positive lens elementand a negative lens element with a concave cemented surface facing theobject side; a second lens unit having negative refractive power; athird lens unit having positive or negative refractive power; a fourthlens unit having positive refractive power; and a last lens unit havingnegative refractive power, wherein, upon zooming from a wide angle endto a telephoto end, at least said first lens unit and said last lensunit move toward the object side so as to increase an air gap betweensaid first lens unit and said second lens unit but to decrease an airgap between said fourth lens unit and said last lens unit, said zoomlens satisfying the following condition:

    0.7<f1/(fw·ft).sup.1/2 <1.4

where f1 is the focal length of said first lens unit, fw is the focallength of the entire lens system at the wide angle end, and ft is thefocal length of the entire lens system at the telephoto end.
 2. A zoomlens according to claim 1, wherein said zoom lens satisfies thefollowing conditions:

    0.08<fw·(N1n-N1p)/|r1m|<0.5

    3< (ν1p-ν1n)

where N1p is the refractive index of said positive lens element in saidfirst lens unit with respect to the d-line, N1n is the refractive indexof said negative lens element in said first lens unit with respect tothe d-line, ν1p is the Abbe number of said positive lens element in saidfirst lens unit with respect to the d-line, ν1n is the Abbe number ofsaid negative lens element in said first lens unit with respect to thed-line, and r1m is the radius of curvature of the concave cementedsurface in said first lens unit.
 3. A zoom lens according to claim 1,wherein said second lens unit includes, on the closest-to-object side, anegative lens element with its concave surface toward the object sideand satisfies the following conditions:

    0.7<fw·(N2n-1)/|r21|<2.0

    43<ν2n

where r21 is the radius of curvature of an object-side surface of saidnegative lens element of said second lens unit, N2n is the refractiveindex of said negative lens element of said second lens unit withrespect to the d-line, and ν2n is the Abbe number of said negative lenselement of said second lens unit with respect to the d-line.
 4. A zoomlens according to claim 1, wherein said last lens unit includes at leastone positive lens element with its concave surface toward the objectside and at least one negative lens element with its concave surfacetoward the object side and satisfies the following conditions:

    0.35<|fe|/fw<0.85

    0.4<ΔBf/(ft-fw)<0.85

where fe is the focal length of said last lens unit, and ΔBf is themoving quantity of said last lens unit upon zooming from the wide angleend to the telephoto end.
 5. A zoom lens according to claim 1, whereinsaid first lens unit and said last lens unit move together upon zoomingfrom the wide angle end to the telephoto end.